We have developed a new type of self-consistent scheme within the approximation, which we call quasiparticle self-consistent (QS). We have shown that QS rather well describes energy bands for a wide-range of materials, including many where the local-density approximation fails. QS contains physical effects found in other theories such as LDA, SIC and in a satisfactory manner without many of their drawbacks (partitioning of itinerant and localized electrons, adjustable parameters, ambiguities in double-counting, etc.). We present some theoretical discussion concerning the formulation of QS, including a prescriptino for calculating the total energy. We also address several key methodological points needed for implementation. We then show convergence checks and some representative results in a variety of materials.

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